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回答二進制所出的 Probability 問題
本貼文共有 47 個回覆
根本看不懂
(a) `bbb(E) [ I( X > K) ] = bbb(P) ( X > K ) = 1 - bbb (P) ( Z le (K - mu)/psi ) = 1 - Phi((K - mu)/psi )`
(b) `bbb(E) [ max( K-X, 0) ] = bbb(E) [ (K-X)^+ ] = int_{ (- oo, K] } ( K - x ) bbb(N)(dx)`
` = int_{ (-oo, K] } ( K - mu ) bbb(N)( dx ) - int_{ (-oo, K] } ( x - mu ) bbb(N)( dx )`
` = (K - mu ) Phi ( (K - mu)/psi ) - int_{ (-oo, (K - mu)/psi ] } psi*x*Phi( dx )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi int_{ ( -oo, (K - mu)/psi] } d( 1/sqrt(2pi)e^(-x^2/2) )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi/sqrt(2pi)exp (-1/2*((K - mu)/psi)^2)`
(c) `bbb(E)[ e^(tx) ] = int_{RR} e^(t*x) bbb(N)(dx)`
` = int_{ RR } 1/sqrt(2 pi psi^2) exp( - ( (x- mu)^2 - 2 psi^2 t x )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) * int_{RR} 1/sqrt(2 pi psi^2) exp( - (( x - (mu + t psi^2))^2 )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) `
(b) `bbb(E) [ max( K-X, 0) ] = bbb(E) [ (K-X)^+ ] = int_{ (- oo, K] } ( K - x ) bbb(N)(dx)`
` = int_{ (-oo, K] } ( K - mu ) bbb(N)( dx ) - int_{ (-oo, K] } ( x - mu ) bbb(N)( dx )`
` = (K - mu ) Phi ( (K - mu)/psi ) - int_{ (-oo, (K - mu)/psi ] } psi*x*Phi( dx )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi int_{ ( -oo, (K - mu)/psi] } d( 1/sqrt(2pi)e^(-x^2/2) )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi/sqrt(2pi)exp (-1/2*((K - mu)/psi)^2)`
(c) `bbb(E)[ e^(tx) ] = int_{RR} e^(t*x) bbb(N)(dx)`
` = int_{ RR } 1/sqrt(2 pi psi^2) exp( - ( (x- mu)^2 - 2 psi^2 t x )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) * int_{RR} 1/sqrt(2 pi psi^2) exp( - (( x - (mu + t psi^2))^2 )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) `
屌你勁撚到, 無論係改板規呢啲戇尻野, 定係數量呢啲認真野都難唔到你
(a) `bbb(E) [ I( X > K) ] = bbb(P) ( X > K ) = 1 - bbb (P) ( Z le (K - mu)/psi ) = 1 - Phi((K - mu)/psi )`
(b) `bbb(E) [ max( K-X, 0) ] = bbb(E) [ (K-X)^+ ] = int_{ (- oo, K] } ( K - x ) bbb(N)(dx)`
` = int_{ (-oo, K] } ( K - mu ) bbb(N)( dx ) - int_{ (-oo, K] } ( x - mu ) bbb(N)( dx )`
` = (K - mu ) Phi ( (K - mu)/psi ) - int_{ (-oo, (K - mu)/psi ] } psi*x*Phi( dx )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi int_{ ( -oo, (K - mu)/psi] } d( 1/sqrt(2pi)e^(-x^2/2) )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi/sqrt(2pi)exp (-1/2*((K - mu)/psi)^2)`
(c) `bbb(E)[ e^(tx) ] = int_{RR} e^(t*x) bbb(N)(dx)`
` = int_{ RR } 1/sqrt(2 pi psi^2) exp( - ( (x- mu)^2 - 2 psi^2 t x )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) * int_{RR} 1/sqrt(2 pi psi^2) exp( - (( x - (mu + t psi^2))^2 )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) `
thx 其實我睇完書已經識做a同c
btw
`bbb(N)(dx)`係代表咩?
(a) `bbb(E) [ I( X > K) ] = bbb(P) ( X > K ) = 1 - bbb (P) ( Z le (K - mu)/psi ) = 1 - Phi((K - mu)/psi )`
(b) `bbb(E) [ max( K-X, 0) ] = bbb(E) [ (K-X)^+ ] = int_{ (- oo, K] } ( K - x ) bbb(N)(dx)`
` = int_{ (-oo, K] } ( K - mu ) bbb(N)( dx ) - int_{ (-oo, K] } ( x - mu ) bbb(N)( dx )`
` = (K - mu ) Phi ( (K - mu)/psi ) - int_{ (-oo, (K - mu)/psi ] } psi*x*Phi( dx )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi int_{ ( -oo, (K - mu)/psi] } d( 1/sqrt(2pi)e^(-x^2/2) )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi/sqrt(2pi)exp (-1/2*((K - mu)/psi)^2)`
(c) `bbb(E)[ e^(tx) ] = int_{RR} e^(t*x) bbb(N)(dx)`
` = int_{ RR } 1/sqrt(2 pi psi^2) exp( - ( (x- mu)^2 - 2 psi^2 t x )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) * int_{RR} 1/sqrt(2 pi psi^2) exp( - (( x - (mu + t psi^2))^2 )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) `
thx 其實我睇完書已經識做a同c![]()
btw
`bbb(N)(dx)`係代表咩?
Gaussian measure with parameters `(mu, psi)`, 我比較懶而用 Lebesgue integration....
我將整個 Real field 當作 Gaussian measure 作量度,事實上是 normal distribution 同無分別...
(a) `bbb(E) [ I( X > K) ] = bbb(P) ( X > K ) = 1 - bbb (P) ( Z le (K - mu)/psi ) = 1 - Phi((K - mu)/psi )`
(b) `bbb(E) [ max( K-X, 0) ] = bbb(E) [ (K-X)^+ ] = int_{ (- oo, K] } ( K - x ) bbb(N)(dx)`
` = int_{ (-oo, K] } ( K - mu ) bbb(N)( dx ) - int_{ (-oo, K] } ( x - mu ) bbb(N)( dx )`
` = (K - mu ) Phi ( (K - mu)/psi ) - int_{ (-oo, (K - mu)/psi ] } psi*x*Phi( dx )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi int_{ ( -oo, (K - mu)/psi] } d( 1/sqrt(2pi)e^(-x^2/2) )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi/sqrt(2pi)exp (-1/2*((K - mu)/psi)^2)`
(c) `bbb(E)[ e^(tx) ] = int_{RR} e^(t*x) bbb(N)(dx)`
` = int_{ RR } 1/sqrt(2 pi psi^2) exp( - ( (x- mu)^2 - 2 psi^2 t x )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) * int_{RR} 1/sqrt(2 pi psi^2) exp( - (( x - (mu + t psi^2))^2 )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) `
thx 其實我睇完書已經識做a同c![]()
btw
`bbb(N)(dx)`係代表咩?
Gaussian measure with parameters `(mu, psi)`, 我比較懶而用 Lebesgue integration....
我將整個 Real field 當作 Gaussian measure 作量度,事實上是 normal distribution 同無分別...
有冇簡單啲嘅方法解呢題?
(a) `bbb(E) [ I( X > K) ] = bbb(P) ( X > K ) = 1 - bbb (P) ( Z le (K - mu)/psi ) = 1 - Phi((K - mu)/psi )`
(b) `bbb(E) [ max( K-X, 0) ] = bbb(E) [ (K-X)^+ ] = int_{ (- oo, K] } ( K - x ) bbb(N)(dx)`
` = int_{ (-oo, K] } ( K - mu ) bbb(N)( dx ) - int_{ (-oo, K] } ( x - mu ) bbb(N)( dx )`
` = (K - mu ) Phi ( (K - mu)/psi ) - int_{ (-oo, (K - mu)/psi ] } psi*x*Phi( dx )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi int_{ ( -oo, (K - mu)/psi] } d( 1/sqrt(2pi)e^(-x^2/2) )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi/sqrt(2pi)exp (-1/2*((K - mu)/psi)^2)`
(c) `bbb(E)[ e^(tx) ] = int_{RR} e^(t*x) bbb(N)(dx)`
` = int_{ RR } 1/sqrt(2 pi psi^2) exp( - ( (x- mu)^2 - 2 psi^2 t x )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) * int_{RR} 1/sqrt(2 pi psi^2) exp( - (( x - (mu + t psi^2))^2 )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) `
thx 其實我睇完書已經識做a同c![]()
btw
`bbb(N)(dx)`係代表咩?
Gaussian measure with parameters `(mu, psi)`, 我比較懶而用 Lebesgue integration....
我將整個 Real field 當作 Gaussian measure 作量度,事實上是 normal distribution 同無分別...
有冇簡單啲嘅方法解呢題?![]()
因為Gaussian distribution 是 L-2 function以及absolutely continuous with respect to Lebesgue measure, 你可以將 `bbb(N) (dx)` 寫成 `1/sqrt(2 pi psi^2) exp( - ( (x- mu)^2 )/(2 psi^2 ) ) dx`
Lebesgue-Stieltjes Integral, Riemann integral 或是 Riemann - Stieltjes integral 答案在這個 case 是無分別....
只不過寫法不同。
屌你勁撚到, 無論係改板規呢啲戇尻野, 定係數量呢啲認真野都難唔到你![]()
andriod無嗰個plugin完全睇唔明
屌你勁撚到, 無論係改板規呢啲戇尻野, 定係數量呢啲認真野都難唔到你![]()
![]()
仆街 睇唔撚明
其實唔知係咩黎
一鍵留名
一鍵留名
(a) `bbb(E) [ I( X > K) ] = bbb(P) ( X > K ) = 1 - bbb (P) ( Z le (K - mu)/psi ) = 1 - Phi((K - mu)/psi )`
(b) `bbb(E) [ max( K-X, 0) ] = bbb(E) [ (K-X)^+ ] = int_{ (- oo, K] } ( K - x ) bbb(N)(dx)`
` = int_{ (-oo, K] } ( K - mu ) bbb(N)( dx ) - int_{ (-oo, K] } ( x - mu ) bbb(N)( dx )`
` = (K - mu ) Phi ( (K - mu)/psi ) - int_{ (-oo, (K - mu)/psi ] } psi*x*Phi( dx )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi int_{ ( -oo, (K - mu)/psi] } d( 1/sqrt(2pi)e^(-x^2/2) )`
` = (K - mu) Phi ( (K - mu)/psi ) + psi/sqrt(2pi)exp (-1/2*((K - mu)/psi)^2)`
(c) `bbb(E)[ e^(tx) ] = int_{RR} e^(t*x) bbb(N)(dx)`
` = int_{ RR } 1/sqrt(2 pi psi^2) exp( - ( (x- mu)^2 - 2 psi^2 t x )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) * int_{RR} 1/sqrt(2 pi psi^2) exp( - (( x - (mu + t psi^2))^2 )/(2 psi^2 ) ) dx`
` = exp ( mu t + 1/2 psi^2 t^2 ) `
thx 其實我睇完書已經識做a同c![]()
btw
`bbb(N)(dx)`係代表咩?
Gaussian measure with parameters `(mu, psi)`, 我比較懶而用 Lebesgue integration....
我將整個 Real field 當作 Gaussian measure 作量度,事實上是 normal distribution 同無分別...
有冇簡單啲嘅方法解呢題?![]()
因為Gaussian distribution 是 L-2 function以及absolutely continuous with respect to Lebesgue measure, 你可以將 `bbb(N) (dx)` 寫成 `1/sqrt(2 pi psi^2) exp( - ( (x- mu)^2 )/(2 psi^2 ) ) dx`
Lebesgue-Stieltjes Integral, Riemann integral 或是 Riemann - Stieltjes integral 答案在這個 case 是無分別....
只不過寫法不同。
好似明明地,thx
我知道啦 密碼係聽日食飯我埋單
多謝哂
多謝哂
小學到中二數學未試過合格
真心好鍾意probit
但係中五雞完全睇唔明
大學讀硬數
但係中五雞完全睇唔明
大學讀硬數
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